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See the Supplemental Material at for a derivation of Eqs. (3) and (4) and detailed expressions of the spin noise power with its limiting behavior for slow and fast intervalley relaxation rates.
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See the Supplemental Material at http://link.aps.org/supplemental/10. 1103/PhysRevLett.113.046602 for a derivation of Eqs. (3) and (4) and detailed expressions of the spin noise power with its limiting behavior for slow and fast intervalley relaxation rates.
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84899747816
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The renormalized (Equation presented) factor has also been recently discussed in,. PRXHAE 2160-3308 10.1103/PhysRevX.4.011034
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The small spin-orbit coupling corrections (Equation presented) to the spin and valley relaxation times are neglected in our phenomenological relaxation time approximation. We expect that such corrections change only the quantitative but not the qualitative features we find.
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The small spin-orbit coupling corrections (Equation presented) to the spin and valley relaxation times are neglected in our phenomenological relaxation time approximation. We expect that such corrections change only the quantitative but not the qualitative features we find.
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Possible correction from intervalley spin-flip scattering, which requires the simultaneous breakdown of time-reversal symmetry and large momentum transfer, is negligible compared to intravalley spin relaxation.
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Possible correction from intervalley spin-flip scattering, which requires the simultaneous breakdown of time-reversal symmetry and large momentum transfer, is negligible compared to intravalley spin relaxation.
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36
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To separate the valley noise contribution from the background photon shot noise, one can measure the shot noise spectrum in the absence of the sample.
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To separate the valley noise contribution from the background photon shot noise, one can measure the shot noise spectrum in the absence of the sample.
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